JPS59635A - Power sensor - Google Patents

Power sensor

Info

Publication number
JPS59635A
JPS59635A JP10971182A JP10971182A JPS59635A JP S59635 A JPS59635 A JP S59635A JP 10971182 A JP10971182 A JP 10971182A JP 10971182 A JP10971182 A JP 10971182A JP S59635 A JPS59635 A JP S59635A
Authority
JP
Japan
Prior art keywords
light
stress
photoelastic
sensor
optical fiber
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP10971182A
Other languages
Japanese (ja)
Other versions
JPS637613B2 (en
Inventor
Michiro Takahashi
道郎 高橋
Masayuki Sato
正之 佐藤
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP10971182A priority Critical patent/JPS59635A/en
Publication of JPS59635A publication Critical patent/JPS59635A/en
Publication of JPS637613B2 publication Critical patent/JPS637613B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L1/00Measuring force or stress, in general
    • G01L1/24Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet
    • G01L1/241Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet by photoelastic stress analysis

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optical Transform (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Abstract

PURPOSE:To stabilize a signal and to obtain an inexpensive power sensor, by using a photoelastic material to form the sensor and detecting a stress condition of the material by utilizing photoelastic phenomena. CONSTITUTION:A sensor is formed by a photoelastic material 9 such as glass, bakelite, epoxy resin etc. and light from a light source 6 polarized by a polarizing board 7 is introduced into a measuring place of the sensor by an optical fiber 8. The intensity of transmitted light of the polarized light is varied by photoelastic phenomena by a stress condition of the material. Said transmitted light is introduced into a photodetecting element 11 by an optical fiber 10. Striped pattern of light and darkness appears in the material by increasing the stress and new pattern appears together with the alteration of the stress. Accordingly, pulse input appears successively in the fiber 10 and is integrated by a counter 12 and the stress is found. For this reason, the signal is stabilized and the inexpensive power sensor is obtained.

Description

【発明の詳細な説明】 本発明は光弾性現象を利用した力センサに関するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a force sensor that utilizes a photoelastic phenomenon.

従来の力センサは、受感部に生ずる歪を抵抗線式歪ゲー
ジに工9検出し、歪の量を増幅して、さらに、そのアナ
ログ童をディジタル変換し、計算機に入力、力の成分を
算出する方式のものが一般的である、 この方式には以下の欠虞がある。
Conventional force sensors use a resistance wire strain gauge to detect the strain that occurs in the sensitive part, amplify the amount of strain, convert the analog value into digital data, input it into a computer, and calculate the force component. This method has the following drawbacks:

(1)歪ゲージの出力は不安定である。(1) The output of the strain gauge is unstable.

(2)増幅器が高価である。(2) Amplifiers are expensive.

(3)  A/D変換器が高価である。(3) A/D converters are expensive.

本発明は従来多用さnている歪ゲージ利用の刀センチに
替わり、光弾性現象を利用して同様の効果を、低価格で
提供しようとするものである。
The present invention aims to provide the same effect at a lower cost by utilizing the photoelastic phenomenon in place of the conventionally widely used knife centimeter using a strain gauge.

以下本発明を図に基づき具体的に説明する。The present invention will be specifically explained below based on the drawings.

第1図に示す工うに、ガラス、ベークライト。The construction shown in Figure 1 is made of sea urchin, glass, and Bakelite.

エポキシ樹脂等の光弾性材料1に、偏光2を透過させる
と透過光は、材料の応力状態にエリ、元の強度が変化す
る。透過光の強さをi、入射さnる偏光をAsinwt
、常備光と異常偏光の位相差をa。
When polarized light 2 is transmitted through a photoelastic material 1 such as an epoxy resin, the original intensity of the transmitted light changes depending on the stress state of the material. The intensity of transmitted light is i, and the incident polarized light is Asinwt.
, the phase difference between the ordinary light and the extraordinary polarized light is a.

入射光と主応力面との傾きをθとすnば1次式が成り立
つ。
If the inclination between the incident light and the principal stress plane is θ, then a linear equation holds true.

そこで。Therefore.

δ−2nπにおいてl−0となる。It becomes l-0 at δ-2nπ.

すなわち透過光の強さを測定することKより。That is, from K, which measures the intensity of transmitted light.

材料に生じた応力状態を仰ることかできる。It can refer to the state of stress that occurs in a material.

第2図に本発明、実施例の外観を、第3図にそのブロッ
ク図を示す。
FIG. 2 shows an external appearance of an embodiment of the present invention, and FIG. 3 shows a block diagram thereof.

光源6を出た元は偏光板にエリ偏光させらnる。The light that exits the light source 6 is polarized by a polarizing plate.

この光を、元ファイバーに工9、そnぞれの応力測定個
所に1で導く。そこで1光弾性材料9を透過した元を再
び光ファイバーにエリ受元素子11に筐で導く。
This light is guided to the original fiber by 9 and 1 to each stress measurement point. Thereupon, the source that has passed through the photoelastic material 9 is guided back into the optical fiber to the edge receiving element 11 through the casing.

光弾性材料の形状、および応力を測定する個所について
は、そnぞn、光センサの仕様に合わせて決定される。
The shape of the photoelastic material and the location where stress is measured are determined in accordance with the specifications of the optical sensor.

さて、第1図のカセンチに荷重が加わった場合を第3図
で説明する。材料中の応力が大きくなるδ につnて1式(υの主応力差にLる81n27−の値が
変化し、材料中に明暗のしま模様があられnる。
Now, the case where a load is applied to the centerpiece shown in FIG. 1 will be explained with reference to FIG. 3. As the stress in the material becomes larger δ, the value of L81n27-, which is the principal stress difference of equation 1 (υ), changes, and a pattern of light and dark stripes appears in the material.

はじめにあられれるし萱を零次のしまと呼ぶが、このし
葦の生ずる場所の近くに受光用光ファイバー10を配置
しである。
First, the hailstones are called zero-order islands, and the light-receiving optical fiber 10 is placed near the place where the hailstones occur.

応力か増すにつf’L、Llが移動し、次々に新しいし
まが生ずる。
As the stress increases, f'L and Ll move, and new stripes are created one after another.

こnを受光素子の出力から見ると、第4図の如く1時間
を共に次々とパルス入力か有ることと等価である。第1
図のカウンター2にLりこのパルス数を積算して応力を
求める。荷重を減する場合にも明暗のしまは同様に発生
するか、1測足個所に対し受元用元ファイバーを2組近
接して設け、明暗のしまの移動1回を検出し、カウンタ
を増減して一対処する。
Looking at this n from the output of the light receiving element, it is equivalent to inputting pulses one after another for one hour as shown in FIG. 1st
The stress is determined by integrating the number of pulses of Lori on the counter 2 in the figure. Even when reducing the load, do bright and dark stripes occur in the same way?Is it possible to install two sets of receiving source fibers close to each other for one foot measurement point, detect one movement of the bright and dark stripes, and increase or decrease the counter? and deal with it.

以上述べた工すに1本発明による刀センナは歪ゲージを
用いないことに↓す、信号の安定化ができ、信頼性が上
ると共に、増幅器、A/Df換器が不要になり、低価格
化か可能となる効果を有する。
One of the above-mentioned features is that the sword sensor according to the present invention does not use strain gauges, so the signal can be stabilized, reliability is improved, and an amplifier and A/Df converter are not required, resulting in low cost. It has the effect of making it possible to

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明に用いる光弾性の原理の説明図。 第2図は本発明の一実施例の外観図、第3図はそのブロ
ック図、第4図は元弾性材の作用を示す説明図、第5図
は受光素子の出力波形図である。 6・・・光源、7・・・偏光板、8・・・元ファイバー
、9・・・光弾性材料、10・・・光ファイバー、11
・・・受光素子、12・・・カウンタ。 代理人弁理士 薄 出 利泗曖豹騙 才 4t!1 畷 才5 図 晴伺t
FIG. 1 is an explanatory diagram of the principle of photoelasticity used in the present invention. FIG. 2 is an external view of one embodiment of the present invention, FIG. 3 is a block diagram thereof, FIG. 4 is an explanatory diagram showing the action of the original elastic material, and FIG. 5 is an output waveform diagram of the light receiving element. 6... Light source, 7... Polarizing plate, 8... Original fiber, 9... Photoelastic material, 10... Optical fiber, 11
... Light receiving element, 12... Counter. Agent Patent Attorney Usui Li Xi Ambiguous Leopard Cheating Talent 4t! 1. Nawsai 5.

Claims (1)

【特許請求の範囲】[Claims] 光源と偏光板と元ファイバーと受光器と光弾性材料を用
いたことを特徴とする力センサ。
A force sensor characterized by using a light source, a polarizing plate, an original fiber, a light receiver, and a photoelastic material.
JP10971182A 1982-06-28 1982-06-28 Power sensor Granted JPS59635A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10971182A JPS59635A (en) 1982-06-28 1982-06-28 Power sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10971182A JPS59635A (en) 1982-06-28 1982-06-28 Power sensor

Publications (2)

Publication Number Publication Date
JPS59635A true JPS59635A (en) 1984-01-05
JPS637613B2 JPS637613B2 (en) 1988-02-17

Family

ID=14517275

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10971182A Granted JPS59635A (en) 1982-06-28 1982-06-28 Power sensor

Country Status (1)

Country Link
JP (1) JPS59635A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0384712U (en) * 1989-12-20 1991-08-28

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56115931A (en) * 1980-02-18 1981-09-11 Toshiba Corp Pressure-measuring device
JPS5744827A (en) * 1980-08-29 1982-03-13 Shimadzu Corp Polarization plane type light pressure sensor

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56115931A (en) * 1980-02-18 1981-09-11 Toshiba Corp Pressure-measuring device
JPS5744827A (en) * 1980-08-29 1982-03-13 Shimadzu Corp Polarization plane type light pressure sensor

Also Published As

Publication number Publication date
JPS637613B2 (en) 1988-02-17

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